US6816237B2 - Imaging optical instrument - Google Patents

Imaging optical instrument Download PDF

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Publication number
US6816237B2
US6816237B2 US10/143,789 US14378902A US6816237B2 US 6816237 B2 US6816237 B2 US 6816237B2 US 14378902 A US14378902 A US 14378902A US 6816237 B2 US6816237 B2 US 6816237B2
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US
United States
Prior art keywords
beams
lens
aperture stop
lens barrel
aperture
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
US10/143,789
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English (en)
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US20020167652A1 (en
Inventor
Kenji Ueyama
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Screen Holdings Co Ltd
Original Assignee
Dainippon Screen Manufacturing Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Dainippon Screen Manufacturing Co Ltd filed Critical Dainippon Screen Manufacturing Co Ltd
Assigned to DAINIPPON SCREEN MFG. CO., LTD. reassignment DAINIPPON SCREEN MFG. CO., LTD. ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: UEYAMA, KENJI
Publication of US20020167652A1 publication Critical patent/US20020167652A1/en
Priority to US10/971,106 priority Critical patent/US6927924B2/en
Application granted granted Critical
Publication of US6816237B2 publication Critical patent/US6816237B2/en
Assigned to SCREEN Holdings Co., Ltd. reassignment SCREEN Holdings Co., Ltd. CHANGE OF NAME (SEE DOCUMENT FOR DETAILS). Assignors: DAINIPPON SCREEN MFG. CO., LTD.
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Classifications

    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B3/00—Simple or compound lenses
    • G02B3/02—Simple or compound lenses with non-spherical faces
    • G02B3/06—Simple or compound lenses with non-spherical faces with cylindrical or toric faces
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00—Optical objectives specially designed for the purposes specified below
    • G02B13/22—Telecentric objectives or lens systems
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B3/00—Simple or compound lenses
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00—Optical elements other than lenses
    • G02B5/001—Axicons, waxicons, reflaxicons
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00—Optical elements other than lenses
    • G02B5/005—Diaphragms
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B7/00—Mountings, adjusting means, or light-tight connections, for optical elements
    • G02B7/02—Mountings, adjusting means, or light-tight connections, for optical elements for lenses
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B7/00—Mountings, adjusting means, or light-tight connections, for optical elements
    • G02B7/02—Mountings, adjusting means, or light-tight connections, for optical elements for lenses
    • G02B7/021—Mountings, adjusting means, or light-tight connections, for optical elements for lenses for more than one lens
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B7/00—Mountings, adjusting means, or light-tight connections, for optical elements
    • G02B7/02—Mountings, adjusting means, or light-tight connections, for optical elements for lenses
    • G02B7/028—Mountings, adjusting means, or light-tight connections, for optical elements for lenses with means for compensating for changes in temperature or for controlling the temperature; thermal stabilisation
    • G—PHYSICS
    • G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
    • G03B27/00—Photographic printing apparatus
    • G03B27/32—Projection printing apparatus, e.g. enlarger, copying camera

Definitions

  • the present invention relates to an imaging optical instrument for imaging light from an object on a recording surface.
  • an imaging optical instrument includes an aperture stop disposed in an optical system for limiting beams contributing to image formation, in order to secure excellent imaging performance or to secure a required focal depth.
  • an aperture stop is formed of a light-shielding sheet of metal or plastic defining a circular or polygonal aperture. The aperture stop is fixed inside a sealed space defined by lenses and a barrel holding the lenses.
  • high power lasers are used as light sources to emit light for forming images on a recording surface
  • light of high energy level enters the optical instrument from the objects.
  • the aperture stop is heated to a high temperature as a result of shielding the high energy light.
  • the heat of the aperture stop reaches the lens barrel by thermal conduction, and may deform the lens barrel locally. Such a deformation disrupts a proper positional relationship between the lenses to lower imaging performance.
  • the heat of the aperture stop filling the lens barrel interior by thermal convection heats up and expands the entire lens barrel. This results in an imaging position shifting along the optical axis.
  • the aperture stop itself may melt or vaporize to lose its light-shielding function.
  • the shielding material may adhere to lens surfaces to lower optical efficiency also.
  • the object of the present invention is to provide an imaging optical instrument capable of effectively preventing an increase in the temperature of an aperture stop.
  • an imaging optical instrument for causing light incident at an entrance end of a lens barrel to pass through an aperture stop and thereafter to leave the lens barrel from an exit end thereof, thereby imaging on a recording surface
  • the aperture stop comprises an optical element having a passage portion formed centrally thereof for allowing passage of beams that should contribute to image formation, and a refracting portion surrounding the passage portion for refracting beams that should be intercepted and causing the beams that should be intercepted to leave the lens barrel from the exit end.
  • This imaging optical instrument is capable of effectively preventing an increase in the temperature of the aperture stop and lens barrel.
  • the aperture stop comprises an optical element having an aperture formed centrally thereof for allowing passage of beams that should contribute to image formation, and a refracting portion surrounding the aperture for refracting beams that should be intercepted and causing the beams that should be intercepted to leave the lens barrel from the exit end. That is, the aperture formed in the optical element is used as the passage portion for allowing passage of the beams.
  • the aperture stop comprises an optical element having a parallel plate portion formed centrally thereof for allowing passage of beams that should contribute to image formation, and a refracting portion surrounding the parallel plate portion for refracting beams that should be intercepted and causing the beams that should be intercepted to leave the lens barrel from the exit end. That is, the parallel plate portion formed in the optical element is used as the passage portion for allowing passage of the beams.
  • an imaging optical instrument for causing light incident at an entrance end of a lens barrel to pass through an aperture stop and thereafter to leave the lens barrel from an exit end thereof, thereby imaging on a recording surface
  • the aperture stop comprises an optical element having an aperture formed centrally thereof for allowing passage of beams that should contribute to image formation, and a reflecting portion surrounding the aperture for reflecting beams that should be intercepted and causing the beams that should be intercepted to leave the lens barrel from the entrance end.
  • an imaging optical instrument for causing light incident at an entrance end of a lens barrel to pass through an aperture stop and thereafter to leave the lens barrel from an exit end thereof, thereby imaging on a recording surface
  • the aperture stop comprises a plurality of light-shielding plates arranged at predetermined intervals along an optical axis of the lens barrel and defining apertures with diameters thereof varying stepwise, the lens barrel defining a vent hole adjacent the aperture stop.
  • FIG. 1 is a sectional side view of an imaging optical instrument in a first embodiment of the invention
  • FIG. 2 is an explanatory view of aperture stops
  • FIG. 3 is a sectional side view of an imaging optical instrument in a second embodiment of the invention.
  • FIG. 4 is a sectional side view of an imaging optical instrument in a third embodiment of the invention.
  • FIG. 5 is an exploded perspective view of an aperture stop in the third embodiment.
  • FIG. 1 is a sectional side view of an imaging optical instrument in a first embodiment of the invention.
  • This imaging optical instrument is designed for causing light emitted from a plurality of light sources 2 arranged adjacent an object to image on a recording surfaces 8 of a photosensitive or thermosensitive material.
  • the imaging optical instrument includes a lens barrel 3 having a lens 4 disposed adjacent an entrance end of the lens barrel 3 and a lens 5 disposed adjacent an exit end of the lens barrel 3 to act as a two-sided telecentric optical system 6 , and an aperture stop 7 .
  • This imaging optical instrument is used, for example, in an image recording apparatus that records images by scanning the photosensitive or thermosensitive material with beams modulated by image signals.
  • the light sources 2 are formed of semiconductor lasers or light emitting diodes, for example. Further, the light sources 2 may be in the form of ends of a plurality of optical fibers connected to semiconductor lasers or light emitting diodes, or a group of openings illuminated by semiconductor lasers or light emitting diodes. These light sources 2 are arranged to emit light having intensity gravities running parallel to one another, and preferably parallel to the optical axis of the two-sided telecentric optical system 6 .
  • the two-sided telecentric optical system 6 includes, in the simplest form, two positive lenses 4 and 5 spaced from each other by a sum of focal lengths thereof.
  • the arrangement of the light sources 2 is magnified or reduced by the two-sided telecentric optical system 6 into an arrangement of luminous points for recording images with a desired resolution on the recording surface 8 . Since the principal rays in the beams emitted from the light sources 2 are parallel to one another, the arrangement of luminous points remains constant even when the recording surface 8 deviates forward or rearward from an imaging plane. Thus, images may be recorded with high precision.
  • the aperture stop 7 is disposed adjacent a meeting point of a rearward focus of the lens 4 and a forward focus of the lens 5 .
  • FIG. 2 is an explanatory view schematically showing various aperture stops 7 a , 7 b and 7 c (which may be referred to collectively as “aperture stop 7 ”).
  • aperture stop 7 Each of FIGS. 2 ( a ), 2 ( b ) and 2 ( c ) includes a side view at left and a front view at right.
  • FIGS. 2 ( a ), 2 ( b ) and 2 ( c ) show various configurations with exaggeration.
  • the aperture stop 7 shown in FIG. 1 corresponds to the aperture stop 7 a shown in FIG. 2 ( a ).
  • the aperture stop 7 a is formed by drilling a plano-convex lens as shown in phantom in the side view at the left of FIG. 2 ( a ).
  • the aperture stop 7 a has an aperture 72 formed centrally thereof to act as a passage of light, and a refracting portion 71 surrounding the aperture 72 to refract the light.
  • the aperture 72 has an inside diameter corresponding to an aperture diameter required of the aperture stop 7 a .
  • This aperture diameter determines an NA (number of apertures) of the beams used in recording images.
  • the aperture diameter is determined by taking optical efficiency and focal depth into account.
  • the parts that should contribute to image formation pass straight through the aperture 72 of the aperture stop 7 a . Consequently, the two-sided telecentric optical system 6 causes these beams to form images of the light sources 2 on the recording surface 8 .
  • the parts that should be intercepted i.e. the parts that should not contribute to image formation
  • the refracting portion 71 of the aperture stop 7 a As shown in hatching in FIG. 1, such parts of the beams, after exiting the lens barrel 3 reach around the imaging points which are formed by the beams having passed through the aperture 72 of the aperture stop 7 a without forming images and without being condensed.
  • the density of light energy in these areas may be made far less than the density of light energy at the imaging point on the recording surface 8 of the light having passed through the aperture 72 of the aperture stop 7 a .
  • an image is recorded without being affected by the light reaching the areas around the imaging point without forming images and without being condensed.
  • the aperture stop 7 a allows the unwanted light to leave the lens barrel 3 from the exit end thereof instead of intercepting such unwanted light. Consequently, this imaging optical instrument effectively avoids the generation of heat occurring in the prior art.
  • the shape of refracting portion 71 of the aperture stop 7 a (i.e. the shape of the plano-convex lens used as stock) must be such that the beams thereby refracted do not impinge on inner walls of the lens barrel 3 , but reach the areas around the imaging point on the recording surface 8 without forming images and without being condensed. Where the refracting portion 71 has an excessively low level of refractive power, the beams having passed through the refracting portion 71 would reach small areas around the imaging point on the recording surface 8 . The density of light energy in these areas is not sufficiently lowered, thereby to produce an adverse effect on image recording.
  • a permissible level of light energy of the beams passing through the refracting portion 71 for producing no adverse effect on image recording is dependent chiefly on the characteristics of a recording medium set to the recording surface 8 .
  • the refracting portion 71 has an excessively high level of refractive power
  • the beams having passed through the refracting portion 71 would impinge on the inner walls of the lens barrel 3 to be absorbed and converted to heat by the inner walls. This gives rise to such problems as deterioration in imaging performance and displacement of an imaging position.
  • a high degree of profile irregularity is not required of the refracting portion 71 of the aperture stop 7 a , which allows the aperture stop 7 a to be manufactured by using an inexpensive plano-convex lens or the like.
  • a large aberration is provided in order to reduce the energy density of the beams reaching areas around an imaging point without forming images and without being condensed.
  • the above aperture stop 7 a may be replaced by the aperture stop 7 b shown in FIG. 2 ( b ) or the aperture stop 7 c shown in FIG. 2 ( c ).
  • the aperture stop 7 b shown in FIG. 2 ( b ) is formed by drilling a cone prism as shown in phantom in the side view at the left of FIG. 2 ( b ).
  • the aperture stop 7 b has an aperture 75 formed centrally thereof, and a refracting portion 74 surrounding the aperture 75 to refract the light.
  • the aperture 75 has an inside diameter corresponding to an aperture diameter required of the aperture stop 7 b.
  • this aperture stop 7 b When this aperture stop 7 b is used, as when the above aperture stop 7 a , is used, of the beams emitted from the light sources 2 , the parts that should contribute to image formation pass straight through the aperture 75 of the aperture stop 7 b . Consequently, the two-sided telecentric optical system 6 causes these beams to form images of the light sources 2 on the recording surface 8 . On the other hand, of the beams emitted from the light sources 2 , the parts that should be intercepted are refracted by the refracting portion 74 of the aperture stop 7 b . Such parts of the beams reach areas around the imaging point without forming images and without being condensed.
  • the beams are in the state of nearly parallel beams where the aperture stop 7 is installed.
  • the aperture stop 7 b obtained by drilling a cone prism is used, variations in the incident angle and exit angle may be reduced. This facilitates optimization of an antireflection coating usually applied to this type of optical element, and assures an improved antireflection effect. Consequently, heat generation adjacent the aperture stop 7 b may be more effectively suppressed than where the foregoing aperture stop 7 a is used.
  • the aperture stop 7 c shown in FIG. 2 ( c ) is formed by cutting and polishing a surface area 79 of a plano-convex lens as shown in phantom in the side view at the left FIG. 2 ( c ).
  • the aperture stop 7 c has a parallel plate portion 78 formed centrally thereof to act as a light passage, and a refracting portion 77 surrounding the parallel plate portion 78 to refract the light.
  • the parallel plate portion 78 has a diameter corresponding to an aperture diameter required of the aperture stop 7 c.
  • this aperture stop 7 c When this aperture stop 7 c is used, as when the above aperture stop 7 a or 7 b is used, of the beams emitted from the light sources 2 , the parts that should contribute to image formation pass straight through the parallel plate portion 78 of the aperture stop 7 c . Consequently, the two-sided telecentric optical system 6 causes these beams to form images of the light sources 2 on the recording surface 8 . On the other hand, of the beams emitted from the light sources 2 , the parts that should be intercepted are refracted by the refracting portion 77 of the aperture stop 7 c . Such parts of the beams reach areas around the imaging point without forming images and without being condensed.
  • aperture stops 7 a and 7 b parts of the beams emitted from light sources 2 arranged off the optical axis could enter the refracting portions 71 and 74 through inner walls of apertures 72 and 75 to be absorbed, scattered or reflected. This would cause a temperature increase adjacent the aperture stops 7 a and 7 b , or lower imaging performance because of flares.
  • the aperture stop 7 c is free from such problems. However, when this aperture stop 7 c is used, the entire system including the parallel plate portion 78 must be designed with aberration corrections.
  • a plano-convex lens or prism is used for the aperture stop 7 .
  • a flattened lens such as a Fresnel lens or graded index lens may be used.
  • a diffracting optical element may be used.
  • FIG. 3 is a sectional side view of an imaging optical instrument in a second embodiment.
  • Like reference numerals are used to identify like parts which are the same as in the first embodiment and will not be described again.
  • the foregoing imaging optical instrument in the first embodiment refracts the beams that should be intercepted and allows these beams to leave the lens barrel 3 from the exit end thereof.
  • the imaging optical instrument in the second embodiment reflects the beams that should be intercepted and allows these beams to leave the lens barrel 3 from the entrance end thereof.
  • This imaging optical instrument employs an aperture stop 7 similar to the aperture stop 7 a shown in FIG. 2 ( a ), and formed of a plano-convex lens having a central aperture, but with a reflective coating 70 applied to the convex surface thereof (opposed to the recording surface 8 shown in FIG. 3 ).
  • the aperture of this aperture stop 7 has an inside diameter corresponding to the aperture diameter required of the aperture stop 7 .
  • the parts that should contribute to image formation pass straight through the aperture of the aperture stop 7 . Consequently, the two-sided telecentric optical system 6 causes these beams to form images of the light sources 2 on the recording surface 8 .
  • the parts that should be intercepted are reflected by the reflective coating 70 on the aperture stop 7 . As shown in hatching in FIG. 3, such parts of the beams leave the lens barrel 3 from the entrance end thereof.
  • the aperture stop 7 allows the unwanted light to leave the lens barrel 3 , from the entrance end thereof in this embodiment, instead of intercepting such light. Consequently, this imaging optical instrument effectively avoids the generation of heat occurring in the prior art.
  • the shape of reflective coating 70 on the aperture stop 7 (i.e. the shape of the plano-convex lens used as stock) must be such that the beams thereby reflected do not impinge on the inner walls of the lens barrel 3 , but exit from the entrance end.
  • a plano-convex lens is used as stock for forming the aperture stop 7 to determine the shape of reflective coating 70 .
  • An element other than a lens may be used.
  • a plane mirror defining a central opening may be used.
  • FIG. 4 is a sectional side view of an imaging optical instrument in a third embodiment.
  • FIG. 5 is an exploded perspective view of an aperture stop in the third embodiment.
  • Like reference numerals are used to identify like parts which are the same as in the first and second embodiments and will not be described again.
  • the imaging optical instruments in the first and second embodiments described hereinbefore cause the beams that should be intercepted to leave the lens barrel 3 from the exit or entrance end thereof.
  • the imaging optical instrument in the third embodiment is constructed to shield and absorb the beams that should be intercepted.
  • an aperture stop 9 employed in the imaging optical instrument in the third embodiment has five thin light-shielding plates 91 , 92 , 93 , 94 and 95 arranged, with spacers 96 in between, along the optical axis of the lens barrel 3 .
  • the five light-shielding plates 91 , 92 , 93 , 94 and 95 define apertures having aperture diameters D 1 , D 2 , D 3 , D 4 and D 5 , respectively.
  • the aperture diameters D 1 , D 2 , D 3 , D 4 and D 5 are progressively smaller from the light-shielding plate 91 to the light-shielding plate 95 .
  • the diameter D 5 of the aperture in the light-shielding plate 95 corresponds to an aperture diameter required of the aperture stop 9 .
  • the lens barrel 3 has an opening formed adjacent the aperture stop 7 , with a filter 31 fitted in the opening for removing foreign matters.
  • the lens barrel 3 has a further opening formed in a position opposed to the above opening, with an exhaust fan 32 fitted therein.
  • each of the light-shielding plates 91 , 92 , 93 , 94 and 95 bears its share in shielding the beams emitted from the light sources 2 .
  • the light-shielding plates 91 , 92 , 93 , 94 and 95 are arranged with the spacers 96 in between, and these spacers 96 have a heat radiating effect comparable to that of heat radiating fins.
  • the light-shielding plates 91 , 92 , 93 , 94 and 95 are prevented from being heated to a high temperature.
  • Air ascending in the lens barrel 3 as a result of heat radiation from the light-shielding plates 91 , 92 , 93 , 94 and 95 is discharged from the lens barrel 3 by the exhaust fan 32 .
  • Fresh air is supplied into the lens barrel 3 through the filter 31 that removes foreign matters. This prevents the interior of the lens barrel 3 from becoming heated to a high temperature.
  • the filter 31 for removing foreign matters effectively prevents dust and the like from entering the lens barrel 3 .
  • the imaging optical instrument according to the invention is applied to an image recording apparatus.
  • the imaging optical instrument according to the invention is not limited to such application.
US10/143,789 2001-05-14 2002-05-14 Imaging optical instrument Expired - Lifetime US6816237B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US10/971,106 US6927924B2 (en) 2001-05-14 2004-10-25 Imaging optical instrument

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
JP2001142585A JP3710724B2 (ja) 2001-05-14 2001-05-14 結像光学装置
JP2001-142585 2001-05-14

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US10/971,106 Expired - Lifetime US6927924B2 (en) 2001-05-14 2004-10-25 Imaging optical instrument

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EP (2) EP1637909B1 (fr)
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DE (1) DE60225867T2 (fr)

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US6927924B2 (en) 2005-08-09
EP1258743A3 (fr) 2004-05-12
EP1637909A2 (fr) 2006-03-22
EP1258743B1 (fr) 2008-04-02
US20020167652A1 (en) 2002-11-14
EP1637909B1 (fr) 2014-04-30
US20050083587A1 (en) 2005-04-21
JP2002341222A (ja) 2002-11-27
EP1637909A3 (fr) 2006-04-12
DE60225867D1 (de) 2008-05-15
DE60225867T2 (de) 2009-04-09

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